Environmental Engineering Reference
In-Depth Information
Klichuvskoi
13
Kizimen
13
Karymsky
13
Eyjafjallajökull
9,13
Kasatochi
8,13
Mutnovsky
Gorely
12,18
Stromboli
5
Mt
Redoubt
13,15
Mt Etna,
e.g.
3,4,5,6
Sarychev
13
Soufrierè Hills
1,5
Sakurajima
2
Popocatépetl
18
Pacaya
11
Masaya
5
San Cristobal
18
Nevado del Ruiz
13
Galeras
Villarica
5
Puyehue-Cordón Caulle
17
Dallafilla, Nabro
13
Ambrym
7,13
Nyiragongo
16
Mt Erebus
10
Figure 8.1 World map of sites where spectroscopic BrO measurements were
performed.
1
Bobrowski
et al
.,
2003
;
2
Lee
et al
.,
2005
;
3
Oppenheimer
et al
.,
2006
;
et al
.,
2009
;
8
Theys
et al
.,
2009
;
9
Heue
et al
.,
2011
;
10
Boichu
et al
.,
2011
;
11
Vogel,
2011
;
13
Hörmann
et al
.,
2013
;
14
Lübcke
15
Kelly
et al
.,
2013
;
16
Bobrowski
et al
., in press;
17
Theys
et al
.,
et al
., 2013;
2014
;
18
this work.
8.2.1 The origin of volcanic halogen species
The source of volcanic halogen emissions can be divided into two categories:
(1)
'
deep
'
volcanic sources, which are associated with melt generation, evolution
and exsolution of vapour and/or hydrosaline
fluids, and
(2) shallow, more secondary sources, which include, e.g., re-volatilisation of
seawater, or other crustal
fluids; and thermal decomposition of hydrothermal
deposits inside the volcano.
The relative importance of both sources still needs to be investigated. Volcanic
halogen
fluxes to the atmosphere are most commonly estimated by two
approaches:
(1) petrological methods (namely melt inclusion studies) on erupted products, and
(2) measurements of halogen to SO
2
ratios combined with SO
2
-
ux measurements
at active or quiescent degassing volcanoes. Both methods have advantages and
disadvantages.